Computer Simulation Technology
 
CST

Transient Simulation of a System-in-Package (SiP)

Courtesy and Permission of  AET Japan, Inc.

This article summarises the simulation of a System-in-Package (SiP) model using the CST MICROWAVE STUDIO® (CST MWS) Transient Solver to determine the S-Parameters, field distribution and system response when excited with  10 and 20 GHz pulses with additional noise signals. An analysis of the SiP with a board mounting and its effect on the is resonant frequency is also performed.


CST MWS System-in-Package model with material definitions
Figure 1: CST MWS System-in-Package model with material definitions

The model, shown in figure 1 and imported from the CDS Cad design System, consists of copper (lossy metal), polyimide and Silicon with bond wires and through vias.The model is initially simulated without the board mounting which will be introduced later in this article.


Definition of the discrete ports in the SiP model
Figure 2: Definition of the discrete ports in the SiP model

Figure 2 shows the discrete port assignment for the power suppy pin (1) and the signal pins (2,3,4,5).


S-Parameters of the unmounted System-in-Package simulation
Figure 3: S-Parameters of the unmounted System-in-Package simulation

Figure 3 shows the S-Parameters of the board without the mounting board. It can be seen that there is a resonance at 10.29 GHz and that the noise coupling factor,  S3,1 , is about -8dB.  


Surface currents in the SiP at 10 GHz for Port 1 excitation - some materials have been hidden for clarity
Figure 4: Surface currents in the SiP at 10 GHz for Port 1 excitation - some materials have been hidden for clarity

As a result of the Time-Domain method, the field at any frequency can be extracted by definition of so-called field monitors. Figure 4 shows an animated field plot of the surface currents at 10GHz as a function of phase. This allows the behaviour of the SiP to be investigated at any user-defined frequencies. The electric field as well as the radiating field can also be visualised.


Board Mounted SiP Model
Figure 5: Board Mounted SiP Model

The next step in the simulation process of the SiP is the addition of the mounting board and the investigation of its effects on the S-Parameters.  Figure 5 shows the model with the mounting board which consists of 3 copper layers and an FR4 substrate. Vias connect the SiP package to the lower copper grounding layer.


Comparison of S-parameters for mounted and unmounted SiP
Figure 6: Comparison of S-parameters for mounted and unmounted SiP

The change in the S-Parameters between the mounted and unmounted SiP models is shown in Figure 6. The resonance, S1,1 , has shifted from 10.29 GHz to a lower frequency of 7.7 GHz and becomes sharper and more singular in nature.


Electric field at a distance of 3m for the mounted and unmounted SiP configurations ( dBuV/m )
Figure 7: Electric field at a distance of 3m for the mounted and unmounted SiP configurations ( dBuV/m )

The electric field was extracted for both simulations via so-called far field monitors which provide field values at user-specified reference distances from the structure. This means that in addition to Signal Integrity analyses, the EMC characteristics of the system-in-package can also be investigated.  Figure 7 shows the increase in the field when the SiP is mounted on the board. This is due to the resonant and almost antenna-like behaviour of the board in the farfield. 

This article has briefly shown how the Time-Domain solver in CST MWS can be applied to the simulation of a System in Package (SiP) and provide broadband S-Parameters and field results as any user-defined frequencies. The E-Field monitors can provide frequency based data in just a single simulation.


CST Article "Transient Simulation of a System-in-Package (SiP)"
last modified 3. Aug 2007 9:58
printed 10. Feb 2012 6:55, Article ID 361
URL:

All rights reserved.
Without prior written permission of CST, no part of this publication may be reproduced by any method, be stored or transferred into an electronic data processing system, neither mechanical or by any other method.

Other Articles

Plasmonic Nano Antennas Simulation with CST MICROWAVE STUDIO®

Plasmonic Nano Antennas Simulation with CST MICROWAVE STUDIO®
This paper is based on: "Comparison of electromagnetic field solvers for the 3D analysis of plasmonic nano antennas" by Johannes Hoffmann, Christian Hafner, Patrick Leidenberger, Jan Hesselbarth, Sven Burger, Proc. SPIE Vol. 7390, pp. 73900J-73900J-11. The Field Distribution inside a 1 nm wide gap between two 80 nm diameter Gold spheres is calculated and compared to a semi analytical reference solution published in the paper. Both general purpose solvers of CST MICROWAVE STUDIO® are used. The simulation results agree closely with the reference solution. Read full article..

Two-Cavity Monotron Particle in Cell (PIC) Simulation

Two-Cavity Monotron Particle in Cell (PIC) Simulation
A monotron is a simple microwave tube which converts DC energy into RF energy. The simulation of such a two-cavity monotron with CST PARTICLE STUDIO® is performed and compared to published results. Read full article..

Consistent Charged Particle Simulation of a Pierce Gun

Consistent Charged Particle Simulation of a Pierce Gun
The pierce type gun example demonstrates the analysis of an electrically large gun configuration using CST PARTICLE STUDIO™ Read full article..

Conductor Backed Coplanar Wave Guide

Conductor Backed Coplanar Wave Guide
This example shows the simulation of a conductor backed coplanar waveguide with a ground via fence for reducing EMI radiation. The excellent agreement between simulation and simulated results can be observed. Read full article..

Design of Circularly-Polarized Patch Antennas using CST MICROWAVE STUDIO®

Design of Circularly-Polarized Patch Antennas using CST MICROWAVE STUDIO®
An RFID Reader Antenna with the following specifications was designed: - Frequency: 908.5 - 914 MHz (In Korea) - VSWR: less than 2 with 50-ohm impedance - Polarization: circular - Axial ratio: less than 3 dB @ 908.5 - 914MHz - Gain: 6 dBi @ 1W transmitted power - Size and weight: as small as possible This article is published with the permission and courtesy of Prof. Bierng-Chearl Ahn and his colleagues at Chungbuk University, Korea. Read full article..

Back